Our target variable is the current in the loop at the instant B = 1.33 T. The direction of
the current is specified by Lenz's law. The magnitude of the current in the loop with
resistance R is given by
I=
Where , the induced emf, is given by Faraday's
law. We need to solve for the time at which B =1.33 T to evaluate
the induced emf and thus the current at this time.
By Lenz's law, the induced current must produce a magnetic fieldinside the loop that is upward, opposing the change in flux from the right-hand rule we described for the direction of the magnetic field produced by a circular loop , which will be in the desired direction if the induced current flows as shown in Fig. 1 in the
Counter clock-wise direction. The magnetic field is uniform over the loop and perpendicular to the plane of the loop, so the magnetic flux is the area of the circular loop. Hence, by Faraday's law the induced a EMFs.
So, the magnitude of the current in the loop is
The time derivative of B is so, we obtain
